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Network Covalent Solids02:18

Network Covalent Solids

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Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
12.9K
Electric Field at the Surface of a Conductor01:26

Electric Field at the Surface of a Conductor

4.6K
Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
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Superconductor01:24

Superconductor

1.9K
A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
1.9K
Types Of Superconductors01:28

Types Of Superconductors

1.7K
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
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Ferromagnetism01:31

Ferromagnetism

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Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.8K
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

2.0K
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
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Video Experimental Relacionado

Updated: May 5, 2026

Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures
08:12

Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures

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Superconductividad en capas bidimensionales de CoO2

Kazunori Takada1, Hiroya Sakurai, Eiji Takayama-Muromachi

  • 1Advanced Materials Laboratory, National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan. takada.kazunori@nims.go.jp

Nature
|March 7, 2003
PubMed
Resumen
Este resumen es generado por máquina.

Los investigadores descubrieron la superconductividad en un nuevo óxido de cobalto en capas, Na(x) CoO2*yH2O. Este hallazgo desafía la creencia de larga data de que las capas de óxido de cobre son esenciales para la superconductividad de alta temperatura de transición (alta Tc).

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Área de la Ciencia:

  • Ciencia de los materiales Ciencia de los materiales.
  • Física de la materia condensada Física de la materia condensada
  • Química del estado sólido.

Sus antecedentes:

  • El descubrimiento de la superconductividad de alta temperatura de transición (alta T ((c)) en óxidos de cobre en capas ha estimulado una extensa investigación sobre fenómenos similares en otros óxidos metálicos en capas.
  • Investigaciones anteriores sobre óxidos metálicos de transición en 3D, incluidos el cobalto y el níquel, no han arrojado superconductividad, lo que lleva a la hipótesis de que las capas de óxido de cobre son indispensables.

Objetivo del estudio:

  • Investigar el potencial de superconductividad en óxidos metálicos en capas más allá de los compuestos a base de cobre.
  • Para explorar las propiedades superconductoras del hidrato de cobalto de sodio (Na(x) CoO2*yH2O).

Principales métodos:

  • Síntesis y caracterización de Na(x) CoO2*yH2O con estequiometría específica (x ≈ 0,35, y ≈ 1,3).
  • Medición de la temperatura de transición superconductora (T ((c)) utilizando técnicas experimentales apropiadas.

Principales resultados:

  • Na(x) CoO2*yH2O fue identificado como un superconductor con una T(c) de aproximadamente 5 K.
  • El compuesto presenta capas bidimensionales de CoO2 separadas por capas aislantes de iones Na+ y moléculas H2O.
  • Las propiedades superconductoras exhiben una fuerte semejanza con las de los óxidos de cobre de alto T.

Conclusiones:

  • El descubrimiento de la superconductividad en Na(x) CoO2*yH2O demuestra que la superconductividad puede ocurrir en los óxidos de cobalto en capas.
  • Las similitudes observadas en las propiedades superconductoras sugieren una física subyacente análoga entre los superconductores de cobalto y cuprato.
  • Este hallazgo amplía el alcance de los materiales que exhiben superconductividad y abre nuevas vías para la investigación en superconductividad no convencional.